Mini Instruments Mini Monitor 900 And 5.40 Series Geiger Counter Manuals Etc
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Mini Instruments Mini Monitor 900 And 5.40 Series Geiger Counter Manuals Etc
- Publication date
- 2019-01-11
- Usage
- Public Domain Mark 1.0


- Topics
- Mini Monitor 900 series, Mini Monitor 5.40, Mini Monitor 5.10, geiger counter, scintillation counter, contamination meter, radiac, survey meter, ratemeter
- Collection
- manual_packs; manuals
- Language
- English
- Item Size
- 8.2G
Mini Instruments Mini Monitor 900 and 5.40 series geiger counter and scintillation counter manuals and related information on calibration, with useful calibration graphs and tables for radiation dose rate response as a function of gamma ray energy, circuit diagrams for repairs, etc. Mini Instruments Ltd was founded in 1963 in the UK, producing light weight compact geiger counters first at 36 Southampton Street, London, WC2, England, before moving to 8 Station Industrial Estate, Burnham on Crouch, Essex, CM0 8RN, England.
The Mark 1-5 instruments (dated 1963-1983) all used two of the bulky PP6 9v batteries, but could also run off the smaller PP9 9v batteries (now used in most smoke detectors) because the battery clips and voltage was the same (although the battery life would be reduced). Their "Radiation and Contamination Monitor Mark 1" in 1963 had no coiled lead, a small meter dial, and no logarithmic scale (just two linear ranges of 0-50, and 0-500 counts/second), and was available with either an end window geiger type (type E) or a side window geiger tube (type S). Following feedback from customers, the Mark 5 appeared in 1970, with coiled probe lead, and a logarithmic scale of 0-2000 counts/second on a large Ferranti meter. The final meter in that series, the 5.10 appeared in 1975, the main difference being a change from the Ferranti meter to the Sifam 32A meter, which has different circuit board threads necessitating a redesign of the Mini Monitor circuit board. An overload circuit was also added, a switching transistor to detect excess current flow in the geiger tube and keep the meter at full scale in high radiation levels where the geiger tube is saturated (causing a fall back in the count rate).
The 900 series (launched in 1983, although earlier models without alarms continued to sell for another five years) needed only one 9v battery, either a PP6, PP9 or a converter box containing 6 AA batteries (6 x 1.5v = 9v). Mini Instruments later incorporated R. A. Stephen's Quartz Fibre Dosimeters brand (after their factory in London closed) and was eventually taken over by first by Morgan, then Nuclear Enterprises (aka NE Technology Ltd), and then in 2003 the Mini Monitor brand became part of Thermo.
Most Nuclear Enterprises scintillation counter probes like the DP2R or BP4 can be directly connected to the PET100 plugs on Mini Monitor 5.40 and 900 series scintillation ratemeter boxes, but note that the voltage and calibration will be different. The Nuclear Enterprises probes contain voltage dividers and capacitors for photomultipliers, but no pre-amplifiers, unlike Mini Monitor scintillation probes.
In addition, as the handbooks point out, the meter scales on the Mini Monitors deliberately do not give the literal pulse per second rate when trying to calibrate with a pulse generator: they instead include a deliberate 100 microsecond circuit response dead time correction. This is trivial at low count rates (below 100 c/s) but approaches 20% at the high end of the logarithmic scale. For example, 4000 pulses per second input is designed to give a Mini Monitor reading of 5000 counts per second, 20% of the counts having occurred during the circuit response dead time of 0.1 ms after a pulse, at this high exposure rate.
If this built-in correction factor on the meter scale is ignored, then attempts to calibrate the instrument using a pulse-generator to give "accurate" readings at the high end of the scale will result in errors of up to 20% at the low range of the scale, because of the randomly timed nature of real radiation pulses means that 20% occur within the dead time of a single pulse at the high end of the range and are thereby counted as a single pulse. (The non-random pulses from the pulse generator cannot overlap, and therefore should NOT be corrected for deadtime, even at the highest range of the scale, unless the product of the dead time per pulse and the count rate per second equals unity!)
Other related information on nuclear radiation monitors calibration, probes, deposited activity to dose rate conversion factors for various nuclides, and the determination of radiation energy using measurements of the shielding factors for beta and gamma rays as a function of radiation energy, is included for reference purposes to help with the interpretation of meter readings in counts per second.
NOTE ON REPAIR OF WINDOWS FOR ALPHA AND BETA (OR DUAL PHOSPHOR ALPHA-BETA) SCINTILLATION PROBES:
Alpha and low energy beta particle scintillation probes have a light-proof window covering the phosphor that must be extremely thin to permit the alpha or low energy beta particles through without stopping them or degrading their energy so much that they can't produce light flashes in the phosphor. 2 micrometre thick aluminised polyester is used, usually two pieces to reduce risk of light entering through pinhole sized defects. This is similar in strength to very delicate tissue paper, is expensive to precision manufacture (about $200 per square metre, each square metre being sufficient to provide two pieces to cover 25 windows in DP6 probes or 50 windows in DP2 probes), and requires time and care to repair a broken probe foil window. Household aluminium foil used for cooking is 16 microns thick and can't be used because it stops alpha particles completely, and low energy beta particles from carbon-14 etc. However, it doesn't stop most of the higher energy beta particles (0.93 MeV mean energy, 2.28 MeV maximum energy) emitted by Yttrium-90, the short-half-life (64 hours) daughter of Strontium-90 (29 years half life), so it can be used in emergency situations where needed for long-term fission product decontamination work after nuclear accidents and explosions (clean up of fission products).
PHOTOMULTIPLIER TUBES
Scintillation probes traditionally use a vacuum photomultiplier tube, either side-wall (like the classic 9-stage 931/931A/931B or the modern 11-stage PB29B03H) or an end-window (like the classic 11-stage 9524B from the 1960s-70s or its modern replacement, the 9924B).
In combination with a suitable phosphor to emit light when hit by alpha or beta particles (where "beta particles" includes Compton electrons released in the material by gamma rays), these can be far more sensitive than geiger counters, and have a smaller "dead time" after each activation than a geiger tube, e.g. 3-10 nanoseconds, compared to about 100 microseconds for a typical sensitive geiger tube.
Most UK Nuclear Enterprises (later NE Technology, now Thermo) scintillation probes originally used 9524B photomultipliers (28mm diameter, 112 mm long end window glass tube, with 26% efficiency at photon detection for 400nm wavelength photons, and a dynode chain current amplification factor ranging from 1 million at 825v to 10 million at 1100v. These were popular because the small diameter meant they fitted well into the "handle" of UK designed ergonomic scintillation probes like the BP4 and DP2.
The 9524B can be directly replaced with the modern 9900B simply by unplugging one photomultiplier from its dynode chain and replacing it with the newer model. However, the 9900B uses lower voltage than the 9524B (the 9900B requires only 750v for 1 million fold current amplification, and 1000v for 10 million). The ADIT designed PB29B03H (used in most Mirion and Canberra smart scintillation probes) is also direcly interchangeable with the 9524B and 9900B, although the PB29B03H is 33mm shorter in length (it has a 79mm long glass tube, compared to 112mm for 9524B and 9900B), but this does not cause a problem in probes where the end window of the photomultiplier is kept in contact with the phosphor window using a large coiled spring in the socket end of the probe.
The ratemeter circuit used for geiger and scintillation probes differ because a photomultiplier produces smaller current pulses than a geiger counter, and therefore requires more amplification. Mini Instruments scintillation probes like the 42 and 44 contain a pre-amplifier to adapt the probe unit for the basic ratemeter circuit, whereas the Nuclear Enterprises probes do not contain a preamplifier, just a dynode chain of resistors and small capacitors to supply 100-150v differences to each of the 11 dynode amplifier stages. Nuclear Enterprises ratemeters and contamination meters use separate circuits (with different switch positions) for geiger and scintillation probes, supplying higher current (lower ratemeter circuit resistance) with less amplification to the geiger tube, and lower current (higher ratemeter circuit resistance) with more amplification to the scintillation probes.
The normal scintillation probe current is about 0.2 microamps, so the scintillation circuits for a 66 megaohm probe dynode chain operating at about 1kV will sound the instrument warning alarm if the current exceeds about 2 microamps, which only occurs if the mylar foil window on the probe is torn, admitting ambient light, or in very high radiation fields which saturate the photomultiplier. Larger currents flow in geiger tubes operating in high radiation levels.
Around 1950 it became clear that a resistance of 1-10 megaohms was needed in a geiger probe which is located at the end of a lengthy cable (not just at the ratemeter end of the cable), to limit the size of the current pulses. Otherwise the entire charge energy stored capacitively within the charged cable at a potential 500-1000v would be driven through the tube every time a count is detected, overheating it in high radiation fields and greatly diminishing the lifetime of the geiger tube (which for small current pulses is typically 100 million counts).
The penalty for increasing the resistance in the geiger probe to reduce current pulse size is that the effective "dead time" of the geiger is increased almost in proportion to the anode resistance, and the amount of amplification required in the ratemeter circuit is increased because the current pulses received by the ratemeter are smaller.
There are various other ratemeter box differences between Nuclear Enterprises ratemeters and Mini Instruments: the former uses a "pulse shaper" circuit to make all geiger pulses similar. Normally geiger tube pulses have random sizes (irrespective of the energy of the alpha or beta particle or gamma ray triggering them); by making all the pulses similar in size, you eliminate this randomness and roughly double effective sensitivity. Mini Instruments circuits were traditionally simpler and did not include a pulse shaper (thus less current used in the circuit and longer battery life, but less accuracy). Mini Instruments circuit contained a current limiter to the loudspeaker, reducing the amplification at high count rates to reduce the noise and also save battery power.
Another development that occurred during the 1970s was the introduction of overload circuits for geiger counters: at very high radiation levels the deadtimes of pulses increasingly overlap so the "count rate" falls back to zero. To prevent confusion, an overload current detection circuit was added to the geiger circuit designs of all instruments for which calibration was required, to prevent the meter falling back at very high radiation currents, which is basically a switching transistor which feeds sufficient current to the meter to maintain a full scale deflection, when the current flowing through the geiger tube is above its 50 microamps or so saturation current (using Ohm's Law V=IR, I = V/R = 500v/10,000,000 ohms = 50 microamps). This is roughly 25 times the maximum permissible current for a photomultiplier based scintillation probe, so the basic geiger circuit is unsuitable for scintillation probes (it would soon burn out the photomultiplier in high radiation fields, by driving too much current through it).
Some key history documents are included. The reader interested in the early use of portable geiger and scintillation counters is also directed to the historic documentary film "Uranium Fever" made by the uranium prospector Raymond Taylor (1955): https://www.youtube.com/watch?v=OdCOOwyE1cE The first portable scintillation counter was invented for uranium prospecting in Canada by Dr Pringle who founded Nuclear Enterprises in Canada and later the UK, to make radiation meters. The great American uranium prospecting rush began with the first Russian nuclear test in August 1949 and ended on New Year's eve, 1970, when the sole buyer of American uranium ore, the U.S. Atomic Energy Commisson announced (due largely to cutbacks in funding prompted by high federal government spending on the Vietnam War and the NASA Apollo Moon program) to stop buying any more uranium ore (it had by then stockpiled enough to last a hundred years). For a less gung-ho view of the uranium rush, please see the typically anti-nuclear biased BBC Earth Science TV propaganda program, "Radioactive Dinosaur Skeletons Have A Dark History", https://www.youtube.com/watch?v=zqfXCmAhymA
Please see also the videos from Oak Ridge National Laboratory physicist Cresson Kearny, showing how, in a radiation emergency, to make your own self-calibrated (by design geometry!) electroscope dosimeter: https://www.youtube.com/watch?v=QD7fW-VBgDA also its testing with radiation at https://www.youtube.com/watch?v=_YHFtPXzW-o and what to do if you measure a lot of radiation: https://www.youtube.com/watch?v=XLyZAVtObLU For a discussion of this, please see our www.nukegate.org page: https://glasstone.blogspot.com/2011/12/
- Addeddate
- 2019-01-11 20:34:56
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UK%20Recovery%20Handbook%20for%20Radiation%20Decontamination%20of%20Inhabited%20Areas.epub
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USNRDL-TR-337%20Decontamination%20procedure%20and%20effectiveness%20for%20farm%20and%20agricultural%20land%20ABSTRACT%20ONLY.epub
USNRDL-TR-570%20Decontamination%20planning%20for%20land%20target%20complexes%20ABSTRACT%20ONLY.epub
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900 series Mini Monitor Radiation dose rate meters R, G and D Instruction Manual_hocr.html download
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495.0B
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Protection against radiations from radium, cobalt-60, and cesium-137_hocr_pageindex.json.gz download
332.0B
RIS-M-2554 Reclamation of urban areas contaminated by fallout_hocr_pageindex.json.gz download
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PAGE NUMBERS JSON
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Electronics magazine September 1987 Build your own geiger counter project_page_numbers.json download
3.6K
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488.0B
USNRDL-TR-335 Wet decontamination procedure effectiveness ABSTRACT ONLY_page_numbers.json download
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900 series Mini Monitor Radiation dose rate meters R, G and D Instruction Manual_jp2.zip download
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